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author | kurchan.jorge <kurchan.jorge@gmail.com> | 2020-12-08 10:32:48 +0000 |
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committer | overleaf <overleaf@localhost> | 2020-12-08 10:32:50 +0000 |
commit | e2084b32773fb240239e70c28956fff9ee370f14 (patch) | |
tree | 8426a66f739461622507db7b7754ddd84bce9933 | |
parent | b128bec287a75df35db8bef28a4df4c480ab9ea5 (diff) | |
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Update on Overleaf.
-rw-r--r-- | bezout.tex | 2 |
1 files changed, 1 insertions, 1 deletions
@@ -218,7 +218,7 @@ Another instrument we have to study this problem is to compute the following par \delta(\sum_i z_i^2-N) \delta\left(\sum_i y_i^2 -N \frac{a-1}{2}\right) \end{equation} The energy $\Re H_0, \Im H_0$ are in a one-to one relation with the temperatures $\beta_R,\beta_I$. The entropy $S(a,H_0) = \ln Z+ +\beta_{R} \langle \Re H_0 \rangle +\beta_I \langle \Im H_0\rangle$ -is the logarithm of thnumber of configurations of a given +is the logarithm of the number of configurations of a given } \bibliographystyle{apsrev4-2} |